Fuel level sensor having dual fluorescent plastic optical fibers

ABSTRACT

An airplane fuel level optical sensor using one side-emitting plastic optical fiber (SPOF) and two fluorescent plastic optical fibers (FPOFs) to detect the airplane fuel level without using any electrically conductive component or element placed inside the fuel tank. This dual-FPOF sensor is capable of achieving high resolution and high accuracy with a one-time calibration in the actual airplane&#39;s fuel tank environment. One embodiment of the dual-FPOF sensor uses one SPOF and two FPOFs to detect fuel level change based on the optical signal output from the two FPOFs. The sensor design uses large-diameter (core and cladding), lightweight, low-cost and high-durability plastic optical fiber, which is very desirable for airplane installation.

BACKGROUND

This disclosure generally relates to systems and methods for measuring a level of liquid in a reservoir, such as a storage tank or other container. More particularly, this disclosure relates to systems and methods for liquid level measurement using an optical sensor.

A need to continuously measure the level of a liquid exists in many commercial and military applications. For example, liquid-level sensors are commonly used in the fuel tanks of airplane, automobiles, and trucks. Liquid-level sensors are also used to monitor liquid levels within storage tanks used for fuel dispensing, wastewater treatment, chemical storage, food processing, etc.

Many transducers for measuring liquid level employ electricity. The electrical output of such transducers changes in response to a change in the liquid level being measured, and is typically in the form of a change in resistance, capacitance, current flow, magnetic field, frequency, and so on. These types of transducers may include variable capacitors or resistors, optical components, Hall Effect sensors, strain gauges, ultrasonic devices, and so on.

Currently most fuel sensors on airplane use electricity. For example, existing electrical capacitance sensors require metallic capacitance plates and metal wiring to be placed inside the tank, which in turn requires complex installations and protection measures to preclude a safety issue under certain electrical fault conditions. This electrical wiring requires careful shielding, bonding, and grounding to minimize stray capacitance and further requires periodic maintenance to ensure electrical contact integrity. Secondly, capacitance probe measurement requires other sensor inputs, such as temperature and density sensor inputs, to supplement the capacitance measurement to accomplish the fuel level sensing.

There is room for improvements in systems and methods that can detect the level of liquid in a fuel tank without introducing electrical current into the fuel tank.

SUMMARY

Fluorescence is the emission of light by a substance that has absorbed light or other electromagnetic radiation. As used herein, the term “fluorescent plastic optical fiber” means a plastic optical fiber that comprises a core surrounded by cladding, wherein the core is doped with special materials that will produce light (i.e., photons) having a first spectral bandwidth centered at a first wavelength when light having a second spectral bandwidth centered at a second wavelength different than the first wavelength is absorbed by that core. Typically the first wavelength is greater than the second wavelength. As used herein, the term “side-emitting plastic optical fiber” means a plastic optical fiber that emits light along the side of the plastic optical fiber. In accordance with alternative embodiments, fluorescent glass optical fibers can be used instead of fluorescent plastic optical fiber.

The subject matter disclosed herein is broadly directed to the design and implementation of an optical liquid level sensor using one side-emitting optical fiber and two fluorescent optical fibers to detect the liquid level without using any electrically conductive component or element placed inside the fuel tank. For the purpose of illustration, the following disclosure is directed to the design and implementation of an airplane fuel level optical sensor using one side-emitting plastic optical fiber (SPOF) and two fluorescent plastic optical fibers (FPOFs) to detect the airplane fuel level without using any electrically conductive component or element placed inside the fuel tank. This dual-FPOF sensor detects the fuel level without the need of using other supplemental sensor inputs, and it is capable of achieving high resolution and high accuracy with a one-time calibration in the actual airplane's fuel tank environment.

More specifically, the dual-FPOF sensor uses one SPOF and two FPOFs having different photo response efficiencies to detect fuel level change based on the optical power signals output from the dual FPOFs. There is no electrical current to pass through the fuel in the tank to cause any safety concern. The sensor design uses large-diameter (core and cladding), lightweight, low-cost and high-durability POF, which is very desirable for airplane installation.

One aspect of the subject matter disclosed in detail below is a system for measuring a level of liquid in a reservoir, comprising: a light source for outputting light; a side-emitting optical fiber having one end optically coupled to the light source; an optical detector for converting impinging light into an electrical signal representing an optical power of the impinging light; and a fluorescent optical fiber positioned parallel to and at a distance from the side-emitting optical fiber and having one end optically coupled to the optical detector. The side-emitting optical fiber and the fluorescent optical fiber may be made of plastic or glass.

In accordance with some embodiments, the system further comprises: a voltage-controlled variable optical attenuator (hereinafter “variable optical attenuator”) that optically couples the fluorescent optical fiber to the optical detector; a computing system that is electrically coupled to the variable optical attenuator; a current-to-voltage converter electrically coupled to receive photo-current output by the optical detector and transmit a voltage to the computing system; and a fuel level indicator electrically coupled to the computing system, wherein the computing system is further configured to output a fuel level to the fuel level indicator, which fuel level is based in part on the voltage received from the current-to-voltage converter.

Another aspect of the subject matter disclosed in detail below is a system for measuring a level of liquid in a reservoir, comprising: a light source for outputting light; a side-emitting optical fiber having one end optically coupled to the light source; first and second optical detectors for converting impinging light into an electrical signal representing an optical power of the impinging light; a first fluorescent optical fiber positioned parallel to and at a distance from the side-emitting optical fiber and having one end optically coupled to the first optical detector; and a second fluorescent optical fiber positioned parallel to and at the distance from the side-emitting optical fiber and having one end optically coupled to the second optical detector, wherein the first and second fluorescent optical fibers have different photo response efficiencies. The side-emitting optical fiber and the fluorescent optical fibers may be made of plastic or glass.

In accordance with some embodiments, the system further comprises: a first variable optical attenuator that optically couples the first fluorescent optical fiber to the first optical detector; a second variable optical attenuator that optically couples the second fluorescent optical fiber to the second optical detector; a light source power controller for controlling the electrical current provided to the light source; and a computing system configured to send first control signals to the first and second variable optical attenuators, which first control signals set the levels of attenuation provided by the first and second variable optical attenuators, and further configured to send second control signals to the light source power controller, which second control signals set the level of electrical current provided to the light source. This system may further comprise: a first current-to-voltage converter coupled to receive photo-current output by the first optical detector and transmit a first voltage to the computing system; and a second current-to-voltage converter coupled to receive photo-current output by the second optical detector and transmit a second voltage to the computing system, wherein the computing system is further configured to calculate a ratio of the first and second voltages, and the first and second control signals are based in part on the ratio. In addition, this system may further comprise a fuel level indicator electrically coupled to the computing system, wherein the computing system is further configured to output a fuel level to the fuel level indicator, which fuel level is based in part on a third voltage received from the first current-to-voltage converter after sending of the first and second control signals.

A further aspect of the subject matter disclosed in detail below is an optical system comprising: first, second and third composite holding rods; first, second and third glass tubes respectively partially embedded in and partially protruding from the first, second and third composite holding rods; a side-emitting plastic optical fiber embedded in the first glass tube; a first fluorescent plastic optical fiber embedded in the second glass tube; a second fluorescent plastic optical fiber embedded in the third glass tube; and a supporting structure that supports the first, second and third composite holding rods such that light emitted by the side-emitting plastic optical fiber will be received by the first and second fluorescent plastic optical fibers.

In accordance with some embodiments, the supporting structure comprises: a composite outer tube having first and second ends; a first end cap affixed to the first end of the composite outer tube; and a second end cap affixed to the second end of the composite outer tube, wherein the first, second and third composite holding rods are disposed inside the composite outer tube. In addition, the optical system may further comprise an optical fiber holding cylinder having first, second and third openings, wherein the first end cap has an opening which is configured to receive the optical fiber holding cylinder, the side-emitting plastic optical fiber passes through the first opening in the optical fiber holding cylinder, the first fluorescent plastic optical fiber passes through the second opening in the optical fiber holding cylinder, and the second fluorescent plastic optical fiber passes through the third opening in the optical fiber holding cylinder. The second end cap has first, second and third openings which are configured to receive respective ends of the first, second and third composite holding rods.

Yet another aspect of the subject matter disclosed in detail below is a method for measuring a height of liquid in a reservoir, comprising: placing a side-emitting optical fiber and a first fluorescent optical fiber in the liquid contained in the reservoir having respective locations whereat the side-emitting optical fiber and the first fluorescent optical fiber are mutually parallel and separated by a distance, and the first fluorescent optical fiber has a first photo response efficiency; inputting light from a light source into one end of the side-emitting optical fiber; side-emitting at least some of the inputted light from the side-emitting optical fiber; absorbing at least some of the side-emitted light inside the first fluorescent optical fiber; producing light by fluorescence inside the first fluorescent optical fiber in response to absorption of side-emitted light; emitting light produced by fluorescence from one end of the first fluorescent optical fiber; converting at least some of the light emitted by the first fluorescent optical fiber into a first photo-current; converting the first photo-current into a first voltage; calculating the height of the liquid in the reservoir based in part on a magnitude of the first voltage; and visually indicating the height on a display.

In accordance with one embodiment of the method, the placing step further comprises placing a second fluorescent optical fiber in the liquid contained in the reservoir having a location whereat the side-emitting optical fiber and the second fluorescent optical fiber are mutually parallel and separated by the distance, and the second fluorescent optical fiber has a second photo response efficiency different than the first photo response efficiency, the method further comprising: absorbing at least some of the side-emitted light inside the second fluorescent optical fiber; producing light by fluorescence inside the second fluorescent optical fiber in response to absorption of side-emitted light; emitting light produced by fluorescence from one end of the second fluorescent optical fiber; converting at least some of the light emitted by the second fluorescent optical fiber into a second photo-current; converting the second photo-current into a second voltage; calculating a ratio of the first and second voltages; and comparing the calculated ratio to a predetermined constant, wherein the height is calculated if the calculated ratio and the predetermined constant are equal. In addition, the method may further comprise: attenuating the light emitted by the first and second fluorescent optical fibers if the calculated ratio and the predetermined constant are not equal; and changing the optical power of the light inputted into the one end of the side-emitting optical fiber if the calculated ratio and the predetermined constant are not equal.

Other aspects of optical sensors suitable for use in detecting the level of a liquid in a reservoir are disclosed and claimed below.

BRIEF DESCRIPTION OF THE DRAWINGS

The features, functions and advantages discussed in the preceding section can be achieved independently in various embodiments or may be combined in yet other embodiments. Various embodiments will be hereinafter described with reference to drawings for the purpose of illustrating the above-described and other aspects.

FIG. 1 is a diagram representing a side-emitting plastic optical fiber and a fluorescent plastic optical fiber separated by a distance d inside a fuel tank.

FIG. 2 is a graph showing results of a laboratory experiment in which optical power output and corresponding jet fuel levels were measured. The data points are indicated by solid circles, while a curve fitting those data points is represented by a dotted line.

FIG. 3 is a diagram representing two fluorescent plastic optical fibers each positioned at distance d from a side-emitting plastic optical fiber inside a fuel tank.

FIG. 4 is a graph showing results of a laboratory experiment in which the ratio of the FPOF optical power outputs (P_(out1)/P_(out2)) produced in response to one SPOF input and corresponding jet fuel levels were measured. The data points are indicated by solid circles, while a curve fitting those data points is represented by a bold line.

FIG. 5 is a diagram representing two fluorescent plastic optical fibers each positioned at distance d from a side-emitting plastic optical fiber inside a fuel tank containing jet fuel with fuel gunk and residue. The fuel gunk and residue are indicated by solid squares.

FIG. 6 is a hybrid diagram showing the design of a dual-FPOF fuel level sensor having an electronics processor configured to compensate for the effects of fuel gunk, residue, POF aging effects and fuel quality variation.

FIG. 7 is a flowchart identifying steps of an iterative algorithm performed by the electronics processor of the dual-FPOF fuel level sensor in accordance with one example.

FIGS. 8 through 17 are diagrams showing a detailed hardware design of a POF assembly in accordance with one embodiment.

FIG. 8 is a diagram representing a perspective view of one SPOF and two FPOFs arranged in parallel with the center axes of the three POFs located at the vertices of an equilateral triangle, major portions of the three POFs being embedded in respective glass tubes.

FIG. 9 is a diagram representing an isometric view of respective ends of the glass tubes with embedded SPOF and FPOFs depicted in FIG. 8, these glass tubes being partly embedded in and partly protruding out of respective composite holding rods.

FIG. 10 is a diagram representing an end view of the composite holding rods (with partially embedded glass tubes) depicted in FIG. 9.

FIG. 11 is a diagram representing a side view of the composite holding rods (with partially embedded glass tubes) depicted in FIGS. 9 and 10.

FIG. 12 is a diagram representing an exploded isometric view of a End-cap assembly comprising three composite holding rods (with partially embedded glass tubes) with end caps at opposite ends thereof.

FIGS. 13 and 14 are diagrams representing plan views of the end caps depicted in FIG. 12.

FIG. 15 is a diagram representing a side view of the End-cap assembly comprising three composite holding rods (with partially embedded glass tubes) with end caps at opposite ends thereof.

FIG. 16 is a diagram representing an isometric view of a POF assembly comprising the end-cap assembly depicted in FIG. 15 and a composite outer tube.

FIG. 17 is a diagram representing a partially sectioned view of the POF assembly depicted in FIG. 16.

Reference will hereinafter be made to the drawings in which similar elements in different drawings bear the same reference numerals.

DETAILED DESCRIPTION

Various embodiments of systems and methods for optical measurement of a level of liquid in a reservoir will now be described in detail for the purpose of illustration. At least some of the details disclosed below relate to optional features or aspects, which in some applications may be omitted without departing from the scope of the claims appended hereto.

In particular, illustrative embodiments of an optical fuel level sensor for airplanes are described in some detail below. However, not all features of an actual implementation are described in this specification. A person skilled in the art will appreciate that in the development of any such actual embodiment, numerous implementation-specific decisions must be made to achieve the developer's specific goals, such as compliance with system-related and business-related constraints, which will vary from one implementation to another. Moreover, it will be appreciated that such a development effort might be complex and time-consuming, but would nevertheless be a routine undertaking for those of ordinary skill in the art having the benefit of this disclosure.

The theoretical underpinning of the fuel level sensor concept disclosed herein will now be described with reference to FIG. 1, which shows a side-emitting plastic optical fiber 4 (hereinafter “SPOF 4”) and a fluorescent plastic optical fiber 6 (hereinafter “FPOF 6”) separated by a distance d inside a fuel tank 2. A typical diameter of SPOF 4 and FPOF 6 is 1 mm. In the configuration depicted in FIG. 1, light having an optical power P_(in) from a light source (not shown) is input to the SPOF 4. In accordance with various embodiments, the primary light source is a high-power blue LED having a center wavelength in the range of 450 to 500 nm or a laser light source having a center wavelength of 455 nm. The horizontal arrows in FIG. 1 represent the propagation of side-emitted light from SPOF 4. The optical power output P_(out) from the FPOF 6 is red light having a center wavelength at 692 nm after absorbing the blue light from the SPOF 4. P_(out) is highest when the fuel tank 2 is empty. As the fuel level rises, P_(out) decreases. By measuring the change in P_(out), the fuel level change can be derived.

In FIG. 1, the following dimensions are indicated: the fuel level is h, and the total length of each of the SPOF 4 and the FPOF 6 is set equal to H, since the end faces of the two POFs are close to the bottom of the fuel tank 2 and H is close to the height of the tank 2. The side-emitting efficiency per unit area of the SPOF 4 is α; Γ is the photo response efficiency of the FPOF 6 per unit area. The detailed mathematical derivation of the relationship of optical power output P_(out) versus fuel level h is described by the following equation: P _(out) =P _(oa) +P _(of) =P _(i)Γ{[α² B(2πr)A _(ff) ]h ³ +[αAA _(fa) −B(2πrα ² H)A _(ff) +αBA _(ff) ]h ²−(2AHαA _(fa))h+αAH ² A _(fa)}  (1) where A=(2πr)²e^(−β) ^(a) ^(d) and B=(2πr)²e^(−β) _(f) ^(d). Physically, as the fuel level changes, P_(out) is the summation of the optical power output (P_(oa)) due to absorption of photons from the SPOF 4 by the air 8 and the optical power output (Pof) due to absorption of photons from the SPOF 4 by the fuel 10. A_(fa) is the effective area of the FPOF 6 that is illuminated by the SPOF 4 in the air 8; A_(ff) is the effective area of the FPOF 6 that is illuminated by the SPOF 4 in the fuel 10; r is the radius of each of the SPOF 4 and the FPOF 6 (r is typically about 1 mm); β_(a) is the absorption coefficient of air as the light emitted from SPOF 4 propagates through the air 8: and β_(f) is the absorption coefficient of fuel as the light emitted from SPOF 4 propagates through the fuel 10.

The theoretical relationship of optical power output P_(out) versus fuel level h as shown in Eq. (1) follows a third-order equation in h. This mathematical correlation was demonstrated by experimental results obtained from jet fuel level measurements in a laboratory. The experimental set-up included a SPOF and a FPOF positioned side by side inside a glass tube. Changes in the jet fuel level inside the glass tube were achieved using a small liquid pumping device connecting a plastic tube from a jet fuel container to the glass tube. With the constant-power output from a blue LED coupled into the SPOF, as the fuel level changed, the optical power output P_(out) of the FPOF was measured with an optical power meter.

FIG. 2 is a graph showing optical power output P_(out) of the FPOF versus fuel level h from those experimental measurements. The data points are indicated by solid circles, while a curve fitting those data points is represented by a dotted line. Each data point plotted on the graph is an ordered pair comprising FPOF optical power output (the ordinate) measured in milliwatts versus jet fuel level measurement (the abscissa) measured in millimeters. The experimental data plotted in FIG. 2 shows optical power output P_(out) versus fuel level h fitted very well with a third-order equation. This confirmed the validity of the theoretical derivation of Eq. (1).

In principle, a single SPOF and a single FPOF should be able to provide the fuel level information based on the detected optical power output P_(out) of the FPOF. But in a real airplane fuel tank, there are issues of fuel gunk and residue which can build up on the surfaces of the SPOF and FPOF. This build-up obscures the fuel level (h) measuring accuracy. Another consideration is that the quality of fuel used in an airplane in service can change over time because different countries may provide different grades of fuel at their airports. In addition, the sensor system should have a stable light source (laser or LED) to provide a proper optical power input P_(in) to the SPOF 4 for measuring fuel level h. Also, over time the POFs can age and the SPOF emitting efficiency (α) and the FPOF response efficiency (Γ) can be degraded over time. To overcome these issues, a second FPOF as reference can be used to build a durable fuel level sensor. A dual-FPOF approach is described as follows.

FIG. 3 shows two FPOFs 6 a and 6 b that are positioned at the same distance d from a SPOF 4 inside a fuel tank 2. The SPOF 4 and the FPOFs 6 a and 6 b have the same radius and length. The SPOF 4 receives the optical power input P_(in). The horizontal arrows in FIG. 3 represent the propagation of side-emitted light from SPOF 4. The first and second FPOFs 6 a and 6 b are designed to have different photo response efficiencies Γ₁ and Γ₂. This can be achieved by different doping of the cores of the FPOFs 6 a and 6 b (e.g., by using different dopants or by using the same dopant at different concentrations). Since the photo response efficiencies Γ₁ and Γ₂ of the FPOFs 6 a and 6 b are different, their respective optical power outputs P_(out1) and P_(out2) will be different.

A wing of an airplane has a height that varies, especially in a spanwise direction. As a consequence, a fuel tank incorporated inside an airplane wing has a height that varies. Typically a wing fuel tank comprises a multiplicity of compartments. It would be desirable to provide fuel level sensors of different lengths which are suitable for installation in fuel tank compartments of different heights. For example, some compartments at the root of a wing may have a height of a few feet, while other compartments near the tip of the wing may have a height of a few inches.

Using the optical power output versus fuel level relationship shown in Eq. (1), the optical power outputs P_(out1) and P_(out2) of the two FPOFs 6 a and 6 b are respectively given by the following equations: P _(out1) =P _(i)Γ₁{[α² B(2πr)A _(ff) ]h ³ +[αAA _(fa) −B(2πrα ² H)A _(ff) +αBA _(ff) ]h ²−(2AHαA _(fa))h+αAH ² A _(fa)}  (2) P _(out2) =P _(i)Γ₂{[α² B(2πr)A _(ff) ]h ³ +[αAA _(fa) −B(2πrα ² H)A _(ff) +αBA _(ff) ]h ²−(2AHαA _(fa))h+αAH ² A _(fa)}  (3) From Eqs. (2) and (3), the following equations can be derived: P _(out2) /P _(out2)=Γ₂/Γ₁   (4) Γ₂/Γ₁ =C ₀₁   (5)

The result of Eq. (4) shows that with two FPOFs, the ratio of their respective optical power outputs is independent of fuel level. The result of Eq. (5) shows that the ratio of the photo response efficiencies Γ₂ and Γ₁ and optical power outputs P_(out2) and P_(out1) is equal to a constant C₀₁. Using Eqs. (2) and (3), the ratio of the photo response efficiencies Γ₂ and Γ₁ can be calculated by measuring the optical power outputs P_(out 1) and P_(out2) for each FPOF at any fuel level h.

FIG. 4 is a graph showing results of a laboratory experiment in which the ratio of the FPOF optical power outputs (P_(out2)/P_(out1)) produced in response to one SPOF optical power input P_(in) and corresponding jet fuel levels were measured. The data points are indicated by solid circles, while a curve fitting those data points is represented by a bold line. Each data point plotted on the graph is an ordered pair comprising optical power output ratio (the ordinate) versus jet fuel level measurement (the abscissa) measured in millimeters. FIG. 4 shows that the optical power output ratio P_(out2)/P_(out1) is very close to a constant that is independent of fuel level. The experimental results shown in FIG. 4 confirm the theory derived in Eqs. (1) to (5).

Using the results from the above analysis, a dual-FPOF sensor was designed and an implementation was proposed as described below.

FIG. 5 is a diagram representing a fuel level optical sensor comprising two FPOF 6 a and 6 b having different photo response efficiencies. Each of the FPOFs 6 a and 6 b is positioned at a distance d from a SPOF 4 inside a fuel tank 2 of an airplane. The fuel tank 2 contains jet fuel 10 with fuel gunk and residue 12 (indicated by small solid squares).

Before operation of the airplane, the installed dual-FPOF fuel level sensor depicted in FIG. 5 should be calibrated. This dual-FPOF fuel level sensor uses one of the FPOFs (e.g., FPOF 6 a) as the measurement POF and the other FPOF (e.g., FPOF 6 b) as the reference POF. During the calibration procedure, the fuel level versus optical power outputs P_(out1) and P_(out 2) are recorded, and the ratio P_(out2)/P_(out1) is calculated and recorded. The resulting value is the constant C₀₁.

Later, during operation of the airplane, the optical power output P_(out1) from the measurement FPOF 6 a is used to indicate the fuel level based on the data from the calibration. But over the lifetime of the sensor being used in the airplane, fuel gunk and residue 12 will be deposited on the SPOF 4 and the FPOFs 6 a and 6 b as shown in FIG. 5, the POFs age over the lifetime of the airplane, and also the fuel quality will vary for an airplane in service. All of these factors may effectively reduce the respective photo response efficiencies Γ₁ and Γ₂ of the two FPOFs 6 a and 6 b. But by using a fuel level electronics processor (not shown in FIG. 5) to continually monitor and regulate the attenuation of the optical power outputs P_(out1) and P_(out2) of the two FPOF 6 a and 6 b and continually adjust the optical power input P_(in) to the SPOF 4, the effects of gunk, residue, POF aging and fuel quality variation can be compensated so that the optical power output P_(out1) versus fuel level measurement is unchanged over the lifetime of the dual-FPOF fuel level sensor being used in the airplane.

Still referring to FIG. 5, the fuel gunk and residue 12 reduces the input optical power that illuminates the surfaces of the FPOFs 6 a and 6 b. The POF aging reduces the SPOF emitting efficiency α and the photo response efficiencies Γ₁ and Γ₂. Similarly, the change in fuel quality also has the same effect in reducing the optical power outputs P_(out1) and P_(out2) of the FPOFs 6 a and 6 b. The design of the dual-FPOF fuel level sensor compensates for the effects of gunk, residue, POF aging and fuel quality variation in part by increasing the optical power input P_(in) to the SPOF 4.

FIG. 6 shows the dual-FPOF design and its electronics processor 20 (or controller), which is configured to achieve stable and reliable fuel level sensing. FIG. 6 also shows the controller electronic functions which are designed to maintain constant ratio of the photo response efficiencies Γ₁ and Γ₂ over the lifetime of the sensor's operation.

As shown in FIG. 6, the output of FPOF 6 a is connected to a first variable optical attenuator 14 a (indicated by the block labeled VOA1), while the output of FPOF 6 b is connected to a second variable optical attenuator 14 b (indicated by the block labeled VOA2). These variable optical attenuators are optical attenuators which attenuate (i.e., reduce the intensity of) the FPOF optical power outputs by applying external voltages. The degree of attenuation can be regulated by changing the magnitudes of the applied external voltages. The regulation of the magnitudes of the external voltages applied to the first and second variable optical attenuators 14 a and 14 b is controlled by respective control signals received from the electronics processor 20 through the electrical connector 22, which is electrically coupled to the electronics processor 20 as shown in FIG. 6.

The one-time calibration is performed while the completed dual-FPOF fuel level sensor is in the airplane's fuel tank 2. During this first calibration, the photo response efficiencies Γ₁and Γ₂ of FPOFs 6 a and 6 b are measured as Γ₀₁ and Γ₀₂ respectively, and then the constant C₀₁ is determined by calculating the ratio Γ₀₂/Γ₀₁. The design of the dual-FPOF fuel level sensor uses FPOF 6 a as the fuel level sensing FPOF and FPOF 6 b as the reference FPOF. Initially, the FPOFs 6 a and 6 b are fabricated such that the photo response efficiency Γ₀₁ of FPOF 6 a is larger than the photo response efficiency Γ₀₂ of FPOF 6 b. During the calibration procedure, electronic digital data representing the fuel levels versus optical power outputs of both P_(out1) and P_(out2) are recorded in a look-up table stored in a non-transitory tangible computer-readable storage medium, such as the non-volatile memory of an electronics processor 20. In addition, a third-order equation is derived that fits the digital calibration data. This third-order equation can be used to interpolate between two stored values in the look-up table when the optical power output P_(out1) is a value between those two stored values. The relationship of fuel level h versus P_(out1) is derived from the measurement data acquired during calibration and stored (as electronic digital data) in the processor's memory.

The FPOFs 6 a and 6 b are respectively connected to the first and second variable optical attenuators 14 a and 14 b. The optical power outputs P_(out1) and P_(out2) from the first and second variable optical attenuators 14 a and 14 b are optically coupled to first and second optical detectors 16 a and 16 b respectively. The magnitude of the signals output by the first and second optical detectors 16 a and 16 b increases monotonically with increasing intensity of light emitted from the ends of FPOFs 6 a and 6 b. The photo-current output from the first optical detector 16 a is electrically coupled to a first transimpedance amplifier 18 a (indicated by the block labeled TIA1) and the photo-current output from the second optical detector 16 b is electrically coupled to a second transimpedance amplifier 18 b (indicated by the block labeled TIA2). A transimpedance amplifier is a current-to-voltage converter, most often implemented using an operational amplifier. The first and second transimpedance amplifiers 18 a and 18 b convert the photo-currents to respective voltages V1 and V2 which are linearly proportional to the optical power outputs P_(out1) and P_(out2) from the first and second variable optical attenuators 14 a and 14 b. The voltages V1 and V2 are applied to respective input ports of the electronics processor 20 through the electrical connector 22 as shown in FIG. 6.

The light source 24 that provides the optical power input P_(in) to the SPOF 4 is either a high-power LED or a laser. In accordance with one embodiment, the light source 24 emits light with a center wavelength of 455 nm (blue), because a light source at this wavelength has high photon energy for optical excitation of the FPOFs 6 a and 6 b. (Additional details concerning the light source are provided below.) The wavelength of the light output by the FPOFs 6 a and 6 b has a narrow spectral bandwidth with a center wavelength of 692 nm (red). The horizontal arrows in FIG. 6 represent light (i.e., photons) propagating from the SPOF 4 to the FPOFs 6 a and 6 b during operation of light source 24. The light source 24 is electrically coupled to a light source power controller 26 (indicated by the block labeled LSPC in FIG. 6) which is configured to stabilize the optical power input P_(in) during variations in temperature and over the lifetime of the dual-FPOF fuel level sensor's operation in response to control signals from the electronics processor 20.

The electronics processor 20 is configured to send the fuel level data to a fuel level indicator 28 in the airplane. The electronics processor 20 may be a dedicated microprocessor or a general-purpose computer, and may calculate the measured level (i.e., height) of the fuel by using a look-up table, a calibration curve, or by solving equations, as appropriate. The fuel level indicator 28 may present information that identifies the amount of fuel present within the fuel tank 2 based on optical power data received by the electronics processor 20. The fuel level indicator 28 may take the form of a display device having a display processor programmed to display the measurement results (e.g., the fuel level) graphically and/or alphanumerically on a display screen.

Still referring to FIG. 6, the electronics processor 20 may be a computer or part of a flight control system located on an airplane. In identifying the amount of fuel present in an irregular-shaped fuel tank, the electronics processor 20 may execute various routines to calculate the amount of fuel present based on optical power data received from respective pairs of FPOFs 6 a and 6 b appropriately placed in various compartments of the fuel tank 2. The fuel information processing software may include routines that take into account the shape of the fuel tank 2 to determine the amount of fuel remaining in the fuel tank 2. The fuel information processing software may further include routines for calibrating processes to form a baseline before a first use or to maintain accuracy of fuel readings. The readings provided by the electronics processor 20 to the fuel level indicator 28 may be integrated or averaged before presentation and may be provided at different time intervals.

FIG. 7 is a flowchart identifying steps of an iterative algorithm performed by the electronics processor 20 in accordance with one example. Based on the above-described fuel level measurement theory and Eqs (4) and (5), the electronics processor 20 is configured to convert the analog voltages V1 and V2 into digital data (step 52) and then calculate the ratio Γ₂/Γ₁=V2/V1=C₁ (step 54). Before sending the fuel level data to the fuel level indicator 28 in the airplane (step 60), the electronics processor 20 determines whether C₁=C₀₁ or not (step 56).

If in step 56 the electronics processor 20 detects that the ratio Γ₂/Γ₁=C₁ does not deviate from the constant C₀₁, the electronics processor 20 uses V1 (which is linearly proportional to P_(out1)) to look up the fuel level h in a lookup table (step 58). If the magnitude of V1 falls between higher and lower values stored in the lookup table, then the previously described third-order equation can be used to calculate the fuel level h. The fuel level h is then output to the fuel level indicator 28 (step 60).

If in step 56 the electronics processor 20 detects that C₁ (equal to the ratio Γ₂/Γ₁) deviates from (i.e., is not equal to) the predetermined constant C₀₁, then the electronics processor 20 increases the optical power input P_(in) through the light source power controller 26, and adjusts the level of attenuation of one or both of the first and second variable optical attenuators 14 a and 14 b to achieve a stable ratio Γ₂/Γ₁. The electronics processor 20 determines whether C₁>C₀₁ or not (step 62).

If C₁>C₀₁, then the electronics processor 20 performs the following calculation (step 64): ΔC ₁=(1/C ₀₁ 1/C ₁)C ₀₁  (6) The electronics processor 20 then generates a control signal instructing the light source power controller 26 to increase the optical power input P_(in) by ΔC₁ (step 66) and a control signal instructing the second variable optical attenuator 14 b to increase attenuation by ΔC₁ (step 68). These adjustment steps are performed iteratively.

Conversely, if C₁ is not greater than C₀₁, then the electronics processor 20 performs the following calculation (step 70): ΔC ₁=(C ₀₁ C ₁)/C ₀₁   (7) The electronics processor 20 then generates a control signal instructing the light source power controller 26 to increase the optical power input P_(in) by ΔC₁ (step 72) and a control signal instructing the first variable optical attenuator 14 a to increase attenuation by ΔC₁ (step 74). These adjustment steps are performed iteratively.

When a ratio Γ₂/Γ₁=C₀₁ is achieved after the iterative process, the electronics processor 20 performs the fuel level calculation (step 58) based on the V1 value from FPOF 6 a and then outputs the fuel level information to the airplane's fuel level indicator 28 (step 60), where V1 is linearly proportional to P_(out1).

An alternative light source selection for the optical power input P_(in) is an ultraviolet light source (e.g., LED or laser) having a wavelength in a range from 200 to 400 nm. An ultraviolet light source has higher photon energy than a blue light source. Therefore the ultraviolet light source increases the photo response efficiencies Γ₁ and Γ₂ of the FPOFs. An ultraviolet light source also has the capability to clear and reduce the amount of gunk and residue deposited on the surfaces of the SPOF and FPOFs, thereby increasing the operating lifetime of the dual-FPOF fuel level sensor.

A detailed hardware design of a POF assembly in accordance with one embodiment is shown in FIGS. 8-17. The fully assembled POF assembly comprises at least the following elements: one SPOF 4, two FPOFs 6 a and 6 b, three glass tubes 30 a-30 c, three composite holding rods 32 a-32 c, two end caps 34 and 36, a composite outer tube 38, and an optical fiber holding cylinder 40.

FIG. 8 shows a perspective view of one SPOF 4 and two FPOFs 6 a and 6 b arranged in parallel with the center axes of the three POFs located at the vertices of an equilateral triangle in accordance with one embodiment. A major portion of the SPOF 4 is embedded in a glass tube 30 a having high strength using optically transparent epoxy with good refractive index matching to the glass tube 30 a. The length of the SPOF 4 is greater than the length of glass tube 30 a, with one end of the SPOF 4 terminating at one end of glass tube 30 a and the other end of the SPOF 4 extending beyond the other end of glass tube 30 a. Similarly, major portions of the FPOFs 6 a and 6 b are embedded in respective glass tubes 30 b and 30 c having high strength using optically transparent epoxy with good refractive index matching to the glass tubes. The length of the FPOF 6 a is greater than the length of glass tube 30 b, with one end of the FPOF 6 a terminating at one end of glass tube 30 b and the other end of the FPOF 6 a extending beyond the other end of glass tube 30 b. Similarly, the length of the FPOF 6 b is greater than the length of glass tube 30 c, with one end of the FPOF 6 b terminating at one end of glass tube 30 c and the other end of the FPOF 6 a extending beyond the other end of glass tube 30 c. The terminal portions of SPOF 4 and FPOFs 6 a and 6 b that extend beyond the glass tubes 30 a-30 c will be referred to hereinafter as “non-embedded portions”.

After embedding major portions of the SPOF 4 and FPOFs 6 a and 6 b inside the glass tubes 30 a-30 c, the three glass tubes 30 a-30 c are seated in respective grooves 33 a-33 c formed in respective composite holding rods 32 a-32 c (see FIG. 9). As seen in FIG. 9, the glass tubes 30 a-30 c are partly embedded in and partly protruding out of the associated composite holding rods 32 a-32 c. The composite holding rods 32 a-32 c support and partially protect the associated glass tubes 30 a-30 c. In accordance with one embodiment, the grooves 33 a-33 c in composite holding rods 32 a-32 c have semicircular profiles with a radius slightly greater than the radius of the glass tubes 30 a-30 c.

FIG. 10 is a diagram representing an end view of the composite holding rods 32 a-32 c positioned and oriented (i.e., located) so that their center axes are positioned at the vertices of a first equilateral triangle T1 (indicated by dashed lines) and the center axes of the SPOF 4 and FPOFs 6 a and 6 b are positioned at the vertices of a second equilateral triangle T2 (indicated by dashed lines) that is inside the first equilateral triangle T1. The vertices of the second equilateral triangle T2 are separated from the respective vertices of the first equilateral triangle T1 by the same distance. In accordance with an alternative embodiment, the composite holding rods 32 a-32 c may be located so that their center axes are positioned at the vertices of an isosceles triangle, with each of the FPOFs 6 a and 6 b being separated from the SPOF 4 by a first distance and the FPOFs 6 a and 6 b being separated from each other by a second distance different than the first distance. As shown in FIG. 10, SPOF 4 and glass tube 30 a are concentric with each other, FPOF 6 a and glass tube 30 b are concentric with each other, and FPOF 6 b and glass tube 30 a are concentric with each other.

In accordance with one example, the elements shown in FIG. 10 have the following dimensions: the SPOF 4 and FPOFs 6 a and 6 b each have a diameter of 1 mm; the glass tubes 30 a-30 c each have a diameter of 2 mm; the composite holding rods 32 a-32 c each have a diameter of 4 mm; the center axis of the respective POF is located off-center from the center axis of the associated composite holding rod by a distance of 2 mm; and the center axes of the FPOFs 6 a and 6 b are separated from the center axis of the SPOF 4 and from each other by a distance of 3.25 mm. In other words, the sides of equilateral triangle T2 having a length of 3.25 mm. These dimensions can be modified based on the airplane's system requirements.

FIG. 11 is a diagram representing a side view of the composite holding rods 32 a-32 c (with partially embedded glass tubes 30 a-30 c) depicted in FIGS. 9 and 10. As seen in FIG. 11, respective non-embedded portions of the SPOF 4 and FPOFs 6 a and 6 b extend beyond the ends of the respective glass tubes 30 a-30 c.

FIG. 12 is a diagram representing an exploded isometric view of a End-cap assembly comprising the components shown in FIGS. 8-11 and additional components, namely, a pair of end caps disposed at opposite ends thereof to hold the composite holding rods 32 a-32 c at their respective locations depicted in FIG. 10. (As used herein, the term “location” comprises position in a fixed three-dimensional coordinate system and orientation relative to that coordinate system.) More specifically, one end of each of the SPOF 4 and FPOFs 6 a and 6 b is held in place by the top end cap 34 and one end of each of the composite holding rods 32 a-2 c is held in place by the bottom end cap 36. The top and bottom end caps 34 and 36 can be either press fit or epoxy bonded to composite holding tubes 32 a-32 c.

As best seen in FIG. 15, the top end cap 34 comprises a first portion 34 a integrally formed with a second portion 34 b. The first portion 34 a has a circular cylindrical outer surface with a first radius; the second portion 34 b has a circular cylindrical outer surface with a second radius less than the first radius. The top end cap 34 can be made from thermoplastic composite materials.

Referring again to FIG. 12, the top end cap 34 has a central opening 46 and two additional openings 48 a and 48 b disposed on opposite sides of opening 46. The openings 46, 48 a and 48 b may be elliptical or oval. All of the openings 46, 48 a and 48 b extend axially through the first and second portions 34 a and 34 b of the top end cap 34.

As best seen in the end view of FIG. 13, an optical fiber holding cylinder 40 is seated in the central opening 46 and has three openings through which the SPOF 4 and FPOFs 6 a and 6 b will be passed. Although the example depicted in FIG. 13 shows an optical fiber holding cylinder 40 having an elliptical shape, the optical fiber holding cylinder 40 may have a geometry other than elliptical.

As seen in FIG. 17, the ends of the SPOF 4 and FPOFs 6 a and 6 b extend through (indicated by dashed lines) and beyond the optical fiber holding cylinder 40. These optical fibers ends will be connected to external optical fibers outside fuel tank 2 by respective optical connectors (not shown in the drawings) at the wall of the fuel tank 2. One of those optical connectors will connect the SPOF 4 to an external optical fiber (not shown in the drawings) that optically couples the SPOF 4 to the light source 24. The other two optical connectors will connect the FPOFs 6 a and 6 b to respective external optical fibers (not shown in the drawings) that optically couple the FPOFs 6 a and 6 b to the first and second variable optical attenuators 14 a and 14 b respectively (shown in FIG. 6).

FIG. 14 is a diagram representing a plan view of the bottom end cap 36. The bottom end cap 36 has a circular cylindrical outer surface with a radius equal to the second radius of the second portion 34 b of the top end cap 34. The bottom end cap 36 can be made from thermoplastic composite materials. The bottom end cap 36 has three openings 42 a-42 c for receiving one end of each of the respective composite holding rods 32 a-32 c with partially embedded glass tubes 30 a-30 c. The openings 42 a-42 c in bottom end cap 36 align and hold the three composite holding rods 32 a-32 c with partially embedded glass tubes 30 a-30 c in the locations depicted in FIG. 10. The bottom end cap 36 further has a pair of openings 44 a and 44 b disposed on opposite sides of the array of three openings 42 a-42 c. All of the openings 42 a-42 c, 44 a and 44 b extend axially through the bottom end cap 36.

Since the SPOF 4 and FPOFs 6 a and 6 b are respectively fixed relative to the composite holding rods 32 a-32 c that hold them, the top and bottom end caps 34 and 36 have the effect of holding the SPOF 4 and FPOFs 6 a and 6 b in alignment at fixed distances from each other. More specifically, the openings 42 a-42 c in the bottom end cap 36 (best seen in FIG. 14) and the openings in the optical fiber holding cylinder 40 hold the SPOF 4 and FPOFs 6 a and 6 b at the desired positions depicted in FIG. 10. Additional structures inside the composite outer tube 38 can be used to support the middle section of each of the embedded SPOF 4 and FPOFs 6 a and 6 b (this structure is not shown in the drawings). The top and bottom end caps 34 and 36, together with the supporting structure inside the composite outer tube 38, enable the SPOF 4 and FPOFs 6 a and 6 b to withstand the extreme vibration and temperature environment in the airplane's fuel tank 2.

FIG. 15 is a diagram representing a side view of the End-cap assembly comprising three composite holding rods 32 a-32 c (with partially embedded glass tubes) having top and bottom end caps 34 and 36 at opposite ends thereof. This End-cap assembly is coupled to the composite outer tube 38 in the manner depicted in FIG. 16, which combination is referred to herein as “the POF assembly”. The composite outer tube 38 is a circular cylindrical tube having an inner radius which is slightly greater than the outer radius of bottom end cap 36 and portion 34 b of top end cap 34. The outer circumferential surface of portion 34 a of top end cap 34 has external threads. The threaded end-cap assembly is screwed into the outer composite tube 38. As seen in FIG. 16, the entire end-cap assembly depicted in FIG. 15 is inserted inside the composite outer tube 38 except for portion 34 a of top end cap 34.

As previously mentioned, FIG. 17 shows a partially sectioned view of the POF assembly depicted in FIG. 16. Only the top end cap 34 and the composite outer tube 38 are shown in section, the section being taken in the plane of the paper as seen in FIG. 17. As seen in FIG. 17, the upper ends of the composite holding rods 32 a-32 c (i.e., the ends on the left-hand side) are seated with a form-fitting relationship inside respective recesses formed in portion 34 b of top end cap 34, three circular feed through holes for the SPOF and the two FPOFs in portion 34 a, while the lower ends of the composite holding rods 32 a-32 c (i.e., the ends on the right-hand side) are seated with a form-fitting relationship inside respective openings 42 a-42 c opening formed in bottom end cap 36. The empty spaces inside the composite outer tube 38 (including the empty space between the glass holding tubes 30 a-30 c disposed within triangle T2 seen in FIG. 10) will be filled with fuel during fuel level measurement. The openings 44 a and 44 b (see FIG. 14) in the bottom end cap 36 allow fuel to flow into the composite outer tube 38 when the POF assembly depicted in FIGS. 16 and 17 is inserted into the airplane fuel tank 2.

Although not shown in the drawings, each optical fiber is a flexible, optically transparent or translucent fiber made of extruded glass or plastic. It can function as a waveguide or light pipe to transmit light between the two ends of the fiber. Optical fibers typically include a transparent or translucent core having a relatively higher index of refraction surrounded by a transparent or translucent cladding material having a relatively lower index of refraction. Light is kept in the core by total internal reflection. This causes the optical fiber to act as a waveguide.

In accordance with the embodiments disclosed herein, the cladding of the SPOF 4 is modified (e.g., by roughening or notching the circumferential surface) to enable a controlled level of radial light side-emitted along the fiber's length. More specifically, the cladding of SPOF 4 may be treated to produce a non-uniform surface in two areas bounded by respective longitudinal slots in a jacket. For example, the outer surface of the cladding may be roughened or notched in two area overlapped by respective longitudinal slots in a jacket, thereby forming two side windows. The cladding of the FPOFs 6 a and 6 b may be modified in a similar manner to form respective side windows that face toward the respective side windows of SPOF 4 when the optical sensor is installed inside a fuel tank 2.

In accordance with the embodiments disclosed herein, the cores of FPOFs 6 a and 6 b have different fluorescing dopants or different concentrations of the same fluorescing dopant such that the photo response efficiencies of the FPOFs 6 a and 6 b will be different. The cores of FPOFs 6 a and 6 b can be activated by light from the SPOF 4 impinging on the side windows of FPOFs 6 a and 6 b and then entering the cores. (Fluorescence occurs when an orbital electron relaxes to its ground state by emitting a photon of light after being excited to a higher quantum state by some type of energy.) The fluorescing dopants produce light which travels along the length of the FPOFs 6 a and 6 b and is then output to the first and second optical detectors 16 a and 16 b by way of the first and second variable optical attenuators 14 a and 14 b respectively.

In the example shown in FIG. 6, optical fibers are used to measure the level of fuel in a fuel tank 2. In other embodiments, the same apparatus may be used to detect other liquids. For example, the system described above may be used to detect the presence of water in a container or hydraulic fluids in a reservoir for a hydraulic system. The illustration of detecting fuel in a fuel tank is presented for purposes of illustration and not meant to limit the manner in which the system shown in FIG. 6 may be used.

The side-emitting optical fiber and the two receiving (fluorescent) optical fibers may include some or all of several enhancements disclosed in U.S. Patent Application Publication No. 2016/0138958, the disclosure of which is incorporated by reference herein in its entirety. For the avoidance of doubt, the following summary of those enhancements will now be provided.

First, a reflective mirror cap may be attached to the bottom end of the side-emitting optical fiber to reflect light back through the side-emitting optical fiber and to prevent light from being lost out the bottom end. A similar reflective cap may be attached to the bottom end of the fluorescent optical fibers to reflect light back through the fluorescent optical fibers toward the attenuators.

Second, the side-emitting optical fiber may further comprise a curved reflective surface disposed between the side-emitting optical fiber and the surrounding jacket. Preferably the jacket is made of a material which is not optically transparent or translucent, such as metal or polymeric material. Similarly, the fluorescent optical fibers may further comprise a curved reflective surface disposed between the fluorescent optical fiber and a surrounding jacket. Preferably the jacket is made of a material which is not optically transparent or translucent, such as metal or polymeric material. In the case where the jacket is made of polymeric material, the jacket can be formed by molding. The side-emitting optical fiber may have a circular, square or hexagonal cross section, with the molded jacket conforming to the shape of the optical fiber.

Third, the side-emitting and fluorescent optical fibers may further comprise respective lenses formed (e.g., by molding) in the longitudinal slots of the respective jackets. Preferably the lenses extend the full length of the longitudinal slots. In combination, a lens and a jacket encase the side-emitting optical fiber, with the lens interfacing with the side window of the side-emitting optical fiber. Similarly, a lens and a jacket encase each fluorescent optical fiber, with the lens interfacing with the side window of fluorescent optical fiber. Preferably the lenses are made of epoxy.

The dual-FPOF fuel level sensors disclosed herein use no metallic components or electrical wiring in the fuel tank. Thus the fuel tank is insulated from electromagnetic interference and lighting effects. As a result of using optical sensors to measure fuel levels, the weight and cost of an airplane can be reduced.

A wing fuel tank system that uses electrical sensors can be retrofitted by substituting the optical sensors disclosed herein. Double shielded electrical wiring for the electrical sensors can be replaced with light and flexible plastic optical fiber, eliminating weight from the wiring and supporting brackets, and eliminating electromagnetic effects from lightning, shorting, fraying of electrical wiring.

While optical fuel level sensors have been described with reference to various embodiments, it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted for elements thereof without departing from the teachings herein. In addition, many modifications may be made to adapt the concepts and reductions to practice disclosed herein to a particular situation. Accordingly, it is intended that the subject matter covered by the claims not be limited to the disclosed embodiments.

The embodiments disclosed above use one or more computing systems. As used in the claims, the term “computing system” comprises one or more of the following which communicate through a network or bus: a computer, a processor (e.g., the electronics processor 20 disclosed herein), a controller, a central processing unit, a microcontroller, a reduced instruction set computer processor, an ASIC, a programmable logic circuit, an FPGA, a digital signal processor, and/or any other circuit or processing device capable of executing the functions described herein. For example, a computing system may comprise multiple microcontrollers or multiple processors which communicate via interfaces.

The methods described herein may be encoded as executable instructions embodied in a non-transitory tangible computer-readable storage medium, including, without limitation, a storage device and/or a memory device. Such instructions, when executed by a processing or computing system, cause the system device to perform at least a portion of the methods described herein.

The process claims set forth hereinafter should not be construed to require that the steps recited therein be performed in alphabetical order (any alphabetical ordering in the claims is used solely for the purpose of referencing previously recited steps) or in the order in which they are recited unless the claim language explicitly specifies or states conditions indicating a particular order in which some or all of those steps are performed. Nor should the process claims be construed to exclude any portions of two or more steps being performed concurrently or alternatingly unless the claim language explicitly states a condition that precludes such an interpretation. 

The invention claimed is:
 1. A system for measuring a level of liquid in a reservoir, comprising: a light source for outputting light; a side-emitting optical fiber having one end optically coupled to the light source; first and second optical detectors for converting impinging light into an electrical signal representing an optical power of the impinging light; a first fluorescent optical fiber positioned parallel to and at a distance from the side-emitting optical fiber and having one end optically coupled to the first optical detector; and a second fluorescent optical fiber positioned parallel to and at the distance from the side-emitting optical fiber and having one end optically coupled to the second optical detector, wherein the first and second fluorescent optical fibers have different photo response efficiencies, a first variable optical attenuator that optically couples the first fluorescent optical fiber to the first optical detector; a second variable optical attenuator that optically couples the second fluorescent optical fiber to the second optical detector; a computing system configured to send first control signals to the first and second variable optical attenuators, which first control signals set the levels of attenuation provided by the first and second variable optical attenuators; a light source power controller for controlling the electrical power provided to the light source, wherein the computing system is further configured to send second control signals to the light source power controller, which second control signals set the level of electrical current provided to the light source, a first current-to-voltage converter coupled to receive photo-current output by the first optical detector and transmit a first voltage to the computing system; and a second current-to-voltage converter coupled to receive photo-current output by the second optical detector and transmit a second voltage to the computing system, wherein the computing system is further configured to calculate a ratio of the first and second voltages, and the first and second control signals are based in part on the ratio.
 2. The system as recited in claim 1, wherein the side-emitting optical fiber and the first and second fluorescent optical fibers are made of plastic.
 3. The system as recited in claim 1, further comprising a fuel level indicator electrically coupled to the computing system, wherein the computing system is further configured to output a fuel level to the fuel level indicator, which fuel level is based in part on a third voltage received from the first current-to-voltage converter after sending of the first and second control signals.
 4. A method for measuring a height of liquid in a reservoir, comprising: placing a side-emitting optical fiber and a first fluorescent optical fiber in the liquid contained in the reservoir having respective locations whereat the side-emitting optical fiber and the first fluorescent optical fiber are mutually parallel and separated by a distance, and the first fluorescent optical fiber has a first photo response efficiency; inputting light from a light source into one end of the side-emitting optical fiber; side-emitting at least some of the inputted light from the side-emitting optical fiber; absorbing at least some of the side-emitted light inside the first fluorescent optical fiber; producing light by fluorescence inside the first fluorescent optical fiber in response to absorption of side-emitted light; emitting light produced by fluorescence from one end of the first fluorescent optical fiber; converting at least some of the light emitted by the first fluorescent optical fiber into a first photo-current; converting the first photo-current into a first voltage; calculating the height of the liquid in the reservoir based in part on a magnitude of the first voltage; and visually indicating the height on a display; wherein the placing step further comprises placing a second fluorescent optical fiber in the liquid contained in the reservoir having a location whereat the side-emitting optical fiber and the second fluorescent optical fiber are mutually parallel and separated by the distance, and the second fluorescent optical fiber has a second photo response efficiency different than the first photo response efficiency, the method further comprising: absorbing at least some of the side-emitted light inside the second fluorescent optical fiber; producing light by fluorescence inside the second fluorescent optical fiber in response to absorption of side-emitted light; emitting light produced by fluorescence from one end of the second fluorescent optical fiber; converting at least some of the light emitted by the second fluorescent optical fiber into a second photo-current; converting the second photo-current into a second voltage; calculating a ratio of the first and second voltages; and comparing the calculated ratio to a predetermined constant, wherein the height is calculated if the calculated ratio and the predetermined constant are equal.
 5. The method as recited in claim 4, further comprising attenuating the light emitted by the first and second fluorescent optical fibers if the calculated ratio and the predetermined constant are not equal.
 6. The method as recited in claim 4, further comprising changing the optical power of the light inputted into the one end of the side-emitting optical fiber if the calculated ratio and the predetermined constant are not equal.
 7. A system for measuring a level of liquid in a reservoir, comprising: a light source for outputting light; a light source power controller for controlling the electrical power provided to the light source, a side-emitting optical fiber having one end optically coupled to the light source; first and second optical detectors for converting impinging light into an electrical signal representing an optical power of the impinging light; a first fluorescent optical fiber positioned parallel to and at a distance from the side-emitting optical fiber and having one end optically coupled to the first optical detector, wherein the first fluorescent optical fiber has a first photo response efficiency; a second fluorescent optical fiber positioned parallel to and at the distance from the side-emitting optical fiber and having one end optically coupled to the second optical detector, wherein the second fluorescent optical fiber has a second photo response efficiency different than the first photo response efficiency; a first current-to-voltage converter configured to convert photo-current output by the first optical detector into a first voltage; a second current-to-voltage converter configured to convert photo-current output by the second optical detector into a second voltage; and a computing system configured to calculate a ratio of the first and second voltages and then send control signals to the light source power controller to set a level of electrical current provided to the light source based at least partly on the calculated ratio.
 8. The system as recited in claim 7, wherein the side-emitting optical fiber and the first and second fluorescent optical fibers are made of plastic.
 9. The system as recited in claim 7, further comprising: a first variable optical attenuator that optically couples the first fluorescent optical fiber to the first optical detector; and a second variable optical attenuator that optically couples the second fluorescent optical fiber to the second optical detector, wherein the computing system is further configured to send control signals to the first and second variable optical attenuators to set the levels of attenuation provided by the first and second variable optical attenuators based at least partly on the calculated ratio. 